As discussed above, \(Y_{B}\) 
depends on the parameters \(\kappa \)  and \(\phi _{\omega }\)  which are responsible for the
generation of the observed value of \(Y_{B}\) , thus we use as their input
ranges \(\left[ -0.1\rightarrow 0.1\right] \)  and \(\left[ 0\rightarrow 2\pi \right] \) , respectively. Then, we plot in the right panel of figure (REF ) the correlation between \(Y_{B}\)  and \(\kappa \)  while the color palette
shows \(\phi _{\omega }\) . We find that the
observed value of \(Y_{B}\)  is predicted for the following ranges of \(\kappa \) 
and \(\phi _{\omega }\) : \(\kappa \in \left[ -0.1\rightarrow -0.0085\right] \cup \left[0.009\rightarrow 0.1\right]\)  and \(0\lesssim \phi _{\omega }\lesssim 6.279\) . We find also that the \(CP\)  conserving values \(\phi _{\omega }=\frac{\pi }{2}\) 
and \(\phi _{\omega }=\frac{3\pi }{2}\)  as well as the regions around them are
excluded. Thus, this source of \(CP\)  violation plays a crucial role in
generating the baryon asymmetry in the present model. A detailed study
concerning the correlation between \(Y_{B}\)  and the other oscillation parameters has
been performed in ref. [1]}.
